Learning the ground state of a non-stoquastic quantum Hamiltonian in a
rugged neural network landscape
- URL: http://arxiv.org/abs/2011.11214v3
- Date: Thu, 17 Jun 2021 09:40:12 GMT
- Title: Learning the ground state of a non-stoquastic quantum Hamiltonian in a
rugged neural network landscape
- Authors: Marin Bukov, Markus Schmitt, Maxime Dupont
- Abstract summary: We investigate a class of universal variational wave-functions based on artificial neural networks.
In particular, we show that in the present setup the neural network expressivity and Monte Carlo sampling are not primary limiting factors.
- Score: 0.0
- License: http://arxiv.org/licenses/nonexclusive-distrib/1.0/
- Abstract: Strongly interacting quantum systems described by non-stoquastic Hamiltonians
exhibit rich low-temperature physics. Yet, their study poses a formidable
challenge, even for state-of-the-art numerical techniques. Here, we investigate
systematically the performance of a class of universal variational
wave-functions based on artificial neural networks, by considering the
frustrated spin-$1/2$ $J_1-J_2$ Heisenberg model on the square lattice.
Focusing on neural network architectures without physics-informed input, we
argue in favor of using an ansatz consisting of two decoupled real-valued
networks, one for the amplitude and the other for the phase of the variational
wavefunction. By introducing concrete mitigation strategies against inherent
numerical instabilities in the stochastic reconfiguration algorithm we obtain a
variational energy comparable to that reported recently with neural networks
that incorporate knowledge about the physical system. Through a detailed
analysis of the individual components of the algorithm, we conclude that the
rugged nature of the energy landscape constitutes the major obstacle in finding
a satisfactory approximation to the ground state wavefunction, and prevents
learning the correct sign structure. In particular, we show that in the present
setup the neural network expressivity and Monte Carlo sampling are not primary
limiting factors.
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